Title: Lincoln D' Carr
1Quantum Phase Transitions in theFermi-Bose
Hubbard model
- Lincoln D. Carr
- JILA
- Physics Department, University of Colorado and
- National Institute for Standards and Technology
- in collaboration with
- Murray Holland
2Motivation Experiments with Cold Atoms on
Lattices
- Exp. realization of Hubbard model
- Parameters m, J, V
- Use of a Feshbach resonance with fermions in the
continuum has led to new states of quantum matter - Strongly interacting Fermi superfluid,
Breached-pair superfluidity, etc. - Problem we address What happens to cold fermions
subject to a Feshbach resonance on a lattice?
3What are Quantum Phase Transitions in the Hubbard
model?
- Hubbard Hamiltonian e.g. bosons
- E.g. cold bosons in a lattice at T0
- Shallow lattice Superfluid phase
- Atoms flow freely
- Phase correlated between sites
- Deep lattice Mott phase
- Atoms confined to individual sites
- Phase uncorrelated between sites
4Our Fermi-Bose Hubbard Hamiltonian
Fermi-pair boson interconversion
Total number of atoms
Chemical equilibrium
5Solve for lowest band, deep lattice
- Consider only paired fermions (Jf ltlt Vf)
- Second order degenerate perturbation theory for
Hf - Hf maps onto new Hamiltonian
-
- Spin operators
- Compare to Heisenberg spin Hamiltonian (XXZ model)
6Two State Approximation and the Phase Diagram
- Same variational wavefunction for each site
- Variational parameters Number angle q and
Mixing angle c - Extremize energy E(q,c).
- Mott insulator superfluid boundary appears as a
saddle point in q.
Fermi-pair/Bose vacuum
One boson, zero Fermi-pairs
Zero bosons, one Fermi-pair
7T0 Phase diagram through crossover
What is a first experimental observable for cold
fermions on a lattice with a Feshbach resonance?
Phase coherence
- (a) n -10 (b) n -1(c) n 1/2(d) n
10NB g1
Mostly bosons
Mostly Fermi-pairs
8Field occupation and avoided crossing
- (a) Mixing anglefor field occupation
- Blue ground state
- Redmaximum
- (b) Avoided crossing in phasediagram
Bosons
Fermi-pairs
9Conclusion
- Proposed general Fermi-Bose Hubbard model which
describes BCS-BEC crossover on a lattice - Recovers Fermi and Bose Hubbard phase
diagramsfor large positive and negative detuning
n - Solved zero to two fermions per site
- Experimental case in 3D 106 fermions, 1003
sites - Both broad and narrow Feshbach resonances
- Predicted clear observable in an experiment
- Phase coherence
- Mott phases consist of dressed Fermi-pairs/bosons
? E-print cond-mat/0501156